Turbulent Combustion in Gas Turbine Engines

Total Page:16

File Type:pdf, Size:1020Kb

Turbulent Combustion in Gas Turbine Engines Lecture 11. Turbulent Combustion in Gas Turbine Engines X.S. Bai TC in Gas Turbines Content • Development of gas turbine • Types of gas turbines • Gas turbine cycle • Gas turbine combustor • New gas turbine combustors for clean environment X.S. Bai TC in Gas Turbines History of gas turbine/jet propulsion engine Hero of Alexandria, Egypt Chinese solid fuel rocket, 1000 AD 130 BC Leonardo Da Vinci’s chimney jack, 1500 Giovanni Branca, Italy, 1629 Isaac Newton’s steam wagon, 1687 Johan Barber made first patent, 1791 X.S. Bai TC in Gas Turbines Gas turbine for modern aviation Frank Whittle, 1930, UK, submitted a patent for a gas turbine for jet propulsion Power Jets Ltd got contract from Air Minsistry In May 1941, the Whittle W1 engine made its first flight X.S. Bai TC in Gas Turbines Gas turbine for modern aviation Gloster Whittle E28 X.S. Bai TC in Gas Turbines Gas turbine for modern aviation Hans von Ohain and Max Hahn, 1936, Germany, submitted a patent for a gas turbine for jet propulsion Ernst Heinkel Aircraft Company made first true jet propulsion aircraft in 1939, Aug - Sept Secundo Campiri, Italy, made a gasturbine engine for the CC-2 aircraft, 1940 American (with the help of the British) made W.IX engine in 1941, GE Later Westinghouse Corporation made contiuous development X.S. Bai TC in Gas Turbines Gas turbine for modern aviation Ohain Whittle X.S. Bai TC in Gas Turbines Rolls-Royce Today •• aero-engines aero-engines •• marine marine propulsionpropulsion systemssystems •• energy energy businessbusiness •• Annual Annual salessales ofof overover £4.5£4.5 billionbillion •• Orders Orders ofof overover £13£13 billionbillion X.S. Bai TC in Gas Turbines Newton’s 3rd Law: principle of propulsion MV Equilibrium Reaction Action Thrust = Mass x Velocity (MV) X.S. Bai TC in Gas Turbines Propeller versus Jet Propulsion Propeller - moves Mvjet LARGE MASS of air at low velocity Mvaircraft Thrust = M(vaircraft -vjet) Thrust = m(Vaircraft -Vjet) Jet - moves small mass of gas at HIGH mVjet mVaircraft VELOCITY X.S. Bai TC in Gas Turbines Jet Engine Layout Compressor Combustion Exhaust Chamber Nozzle mVaircraft mVjet Shaft Turbine ’Straight-through’ configuration X.S. Bai TC in Gas Turbines Different Jet Engine Types CivilCivil turbofanturbofan -- TrentTrent MilitaryMilitary turbofanturbofan -- EJ200EJ200 X.S. Bai TC in Gas Turbines Reverse Thrust NetNet 25%25% toto 30%30% thrustthrust 85%85% thrustthrust 15%15% thrustthrust X.S. Bai TC in Gas Turbines Gas turbine cycle: Brayton cycle 40 Pressure (atmospheres) Expansion/ Power 0 1500 Temperature (degrees C) 0 intake compression combustion exhaust X.S. Bai TC in Gas Turbines Gas turbine cycle: Brayton cycle TR: temperature ratio a-b PR: pressure ratio a-b X.S. Bai TC in Gas Turbines Trend of gas turbine development X.S. Bai TC in Gas Turbines Gas turbine running conditions X.S. Bai TC in Gas Turbines Gas turbine combustor • Stright pipe • Diffuser • Flame stabilization • Optimal air supply X.S. Bai TC in Gas Turbines Combustor Operation X.S. Bai TC in Gas Turbines Jet Engine Layout Can combustor Whittle W1 engine, 1941 X.S. Bai TC in Gas Turbines Turbulent flame shape and flame height (3) order of estimation During time Δt, fuel molecule is convected R from inlet to the tip of flame at a speed U, and oxygen molecule is transport by turbulence from air stream to the flame tip u’ at a speed u’. U H H R Δt ∝ ∝ U u' 2R RU R ⇒ H ∝ ∝ u' I I=u’/U: intensity of turbulence X.S. Bai TC in Gas Turbines Recall: Laminar flame shape and flame height - order of estimation During time Δt, fuel molecule is convected R from inlet to the tip of flame at a speed U, and oxygen molecule is diffused from air stream to the flame tip. D is diffusion coef. U H H R2 Δt ∝ ∝ U D R2U 2R ⇒ H ∝ D X.S. Bai TC in Gas Turbines Dependence of flame height on injection speed U 2R X.S. Bai TC in Gas Turbines Dependence of flame height on burner diameter H laminar turbulent U R 2R ... X.S. Bai TC in Gas Turbines Jet Engine Layout Annular cannular X.S. Bai TC in Gas Turbines Combustor Operation Primary zone Dilution zone Intermediate zone Fuel spray nozzle X.S. Bai TC in Gas Turbines Reverse flow combustor X.S. Bai TC in Gas Turbines Development of modern gas turbine for clean environment X.S. Bai TC in Gas Turbines General consideration 100 30 temperature range for 25 80 low emissions 20 60 NOx 15 CO 40 10 carbon monoxide, ppmv 20 oxides of nitrogen, ppmv 5 0 0 1600 1700 1800 1900 2000 primary temperature, K X.S. Bai TC in Gas Turbines Other cocnepts • Variable geometry • Dry low NOx (DLN) combustion & lean prevaporized premixed (LPP) combustion • Humid air combustion • Rich burner, quick quench, lean burn (RQL) (premixed) • Catalytic combustion • Flameless combustion X.S. Bai TC in Gas Turbines Diffusion Flames X.S. Bai TC in Gas Turbines FLOX X.S. Bai TC in Gas Turbines Flameless: air staged combustion X.S. Bai TC in Gas Turbines Flames and flameless flames FLOX X.S. Bai TC in Gas Turbines Flames and FLOX X.S. Bai TC in Gas Turbines Flames and flameless X.S. Bai TC in Gas Turbines.
Recommended publications
  • Failure Analysis of Gas Turbine Blades in a Gas Turbine Engine Used for Marine Applications
    INTERNATIONAL JOURNAL OF International Journal of Engineering, Science and Technology MultiCraft ENGINEERING, Vol. 6, No. 1, 2014, pp. 43-48 SCIENCE AND TECHNOLOGY www.ijest-ng.com www.ajol.info/index.php/ijest © 2014 MultiCraft Limited. All rights reserved Failure analysis of gas turbine blades in a gas turbine engine used for marine applications V. Naga Bhushana Rao1*, I. N. Niranjan Kumar2, K. Bala Prasad3 1* Department of Marine Engineering, Andhra University College of Engineering, Visakhapatnam, INDIA 2 Department of Marine Engineering, Andhra University College of Engineering, Visakhapatnam, INDIA 3 Department of Marine Engineering, Andhra University College of Engineering, Visakhapatnam, INDIA *Corresponding Author: e-mail: [email protected] Tel +91-8985003487 Abstract High pressure temperature (HPT) turbine blade is the most important component of the gas turbine and failures in this turbine blade can have dramatic effect on the safety and performance of the gas turbine engine. This paper presents the failure analysis made on HPT turbine blades of 100 MW gas turbine used in marine applications. The gas turbine blade was made of Nickel based super alloys and was manufactured by investment casting method. The gas turbine blade under examination was operated at elevated temperatures in corrosive environmental attack such as oxidation, hot corrosion and sulphidation etc. The investigation on gas turbine blade included the activities like visual inspection, determination of material composition, microscopic examination and metallurgical analysis. Metallurgical examination reveals that there was no micro-structural damage due to blade operation at elevated temperatures. It indicates that the gas turbine was operated within the designed temperature conditions. It was observed that the blade might have suffered both corrosion (including HTHC & LTHC) and erosion.
    [Show full text]
  • Progress and Challenges in Liquid Rocket Combustion Stability Modeling
    Seventh International Conference on ICCFD7-3105 Computational Fluid Dynamics (ICCFD7), Big Island, Hawaii, July 9-13, 2012 Progress and Challenges in Liquid Rocket Combustion Stability Modeling V. Sankaran∗, M. Harvazinski∗∗, W. Anderson∗∗ and D. Talley∗ Corresponding author: [email protected] ∗ Air Force Research Laboratory, Edwards AFB, CA, USA ∗∗ Purdue University, West Lafayette, IN, USA Abstract: Progress and challenges in combustion stability modeling in rocket engines are con- sidered using a representative longitudinal mode combustor developed at Purdue University. The CVRC or Continuously Variable Resonance Chamber has a translating oxidizer post that can be used to tune the resonant modes in the chamber with the combustion response leading to self- excited high-amplitude pressure oscillations. The three-dimensional hybrid RANS-LES model is shown to be capable of accurately predicting the self-excited instabilities. The frequencies of the dominant rst longitudinal mode as well as the higher harmonics are well-predicted and their rel- ative amplitudes are also reasonably well-captured. Post-processing the data to obtain the spatial distribution of the Rayleigh index shows the existence of large regions of positive coupling be- tween the heat release and the pressure oscillations. Dierences in the Rayleigh index distribution between the fuel-rich and fuel-lean cases appears to correlate well with the observation that the fuel-rich case is more unstable than the fuel-lean case. Keywords: Combustion Instability, Liquid Rocket Engines, Reacting Flow. 1 Introduction Combustion stability presents a major challenge to the design and development of liquid rocket engines. Instabilities are usually the result of a coupling between the combustion dynamics and the acoustics in the combustion chamber.
    [Show full text]
  • Aerospace Engine Data
    AEROSPACE ENGINE DATA Data for some concrete aerospace engines and their craft ................................................................................. 1 Data on rocket-engine types and comparison with large turbofans ................................................................... 1 Data on some large airliner engines ................................................................................................................... 2 Data on other aircraft engines and manufacturers .......................................................................................... 3 In this Appendix common to Aircraft propulsion and Space propulsion, data for thrust, weight, and specific fuel consumption, are presented for some different types of engines (Table 1), with some values of specific impulse and exit speed (Table 2), a plot of Mach number and specific impulse characteristic of different engine types (Fig. 1), and detailed characteristics of some modern turbofan engines, used in large airplanes (Table 3). DATA FOR SOME CONCRETE AEROSPACE ENGINES AND THEIR CRAFT Table 1. Thrust to weight ratio (F/W), for engines and their crafts, at take-off*, specific fuel consumption (TSFC), and initial and final mass of craft (intermediate values appear in [kN] when forces, and in tonnes [t] when masses). Engine Engine TSFC Whole craft Whole craft Whole craft mass, type thrust/weight (g/s)/kN type thrust/weight mini/mfin Trent 900 350/63=5.5 15.5 A380 4×350/5600=0.25 560/330=1.8 cruise 90/63=1.4 cruise 4×90/5000=0.1 CFM56-5A 110/23=4.8 16
    [Show full text]
  • Noise Reduction Technologies for Turbofan Engines
    NASA/TM—2007-214495 Noise Reduction Technologies for Turbofan Engines Dennis L. Huff Glenn Research Center, Cleveland, Ohio September 2007 NASA STI Program . in Profile Since its founding, NASA has been dedicated to the • CONFERENCE PUBLICATION. Collected advancement of aeronautics and space science. The papers from scientific and technical NASA Scientific and Technical Information (STI) conferences, symposia, seminars, or other program plays a key part in helping NASA maintain meetings sponsored or cosponsored by NASA. this important role. • SPECIAL PUBLICATION. Scientific, The NASA STI Program operates under the auspices technical, or historical information from of the Agency Chief Information Officer. It collects, NASA programs, projects, and missions, often organizes, provides for archiving, and disseminates concerned with subjects having substantial NASA’s STI. The NASA STI program provides access public interest. to the NASA Aeronautics and Space Database and its public interface, the NASA Technical Reports Server, • TECHNICAL TRANSLATION. English- thus providing one of the largest collections of language translations of foreign scientific and aeronautical and space science STI in the world. technical material pertinent to NASA’s mission. Results are published in both non-NASA channels and by NASA in the NASA STI Report Series, which Specialized services also include creating custom includes the following report types: thesauri, building customized databases, organizing and publishing research results. • TECHNICAL PUBLICATION. Reports of completed research or a major significant phase For more information about the NASA STI of research that present the results of NASA program, see the following: programs and include extensive data or theoretical analysis. Includes compilations of significant • Access the NASA STI program home page at scientific and technical data and information http://www.sti.nasa.gov deemed to be of continuing reference value.
    [Show full text]
  • Propulsion Systems for Aircraft. Aerospace Education II
    . DOCUMENT RESUME ED 111 621 SE 017 458 AUTHOR Mackin, T. E. TITLE Propulsion Systems for Aircraft. Aerospace Education II. INSTITUTION 'Air Univ., Maxwell AFB, Ala. Junior Reserve Office Training Corps.- PUB.DATE 73 NOTE 136p.; Colored drawings may not reproduce clearly. For the accompanying Instructor Handbook, see SE 017 459. This is a revised text for ED 068 292 EDRS PRICE, -MF-$0.76 HC.I$6.97 Plus' Postage DESCRIPTORS *Aerospace 'Education; *Aerospace Technology;'Aviation technology; Energy; *Engines; *Instructional-. Materials; *Physical. Sciences; Science Education: Secondary Education; Textbooks IDENTIFIERS *Air Force Junior ROTC ABSTRACT This is a revised text used for the Air Force ROTC _:_progralit._The main part of the book centers on the discussion -of the . engines in an airplane. After describing the terms and concepts of power, jets, and4rockets, the author describes reciprocating engines. The description of diesel engines helps to explain why theseare not used in airplanes. The discussion of the carburetor is followed byan explanation of the lubrication system. The chapter on reaction engines describes the operation of,jets, with examples of different types of jet engines.(PS) . 4,,!It********************************************************************* * Documents acquired by, ERIC include many informal unpublished * materials not available from other souxces. ERIC makes every effort * * to obtain the best copravailable. nevertheless, items of marginal * * reproducibility are often encountered and this affects the quality * * of the microfiche and hardcopy reproductions ERIC makes available * * via the ERIC Document" Reproduction Service (EDRS). EDRS is not * responsible for the quality of the original document. Reproductions * * supplied by EDRS are the best that can be made from the original.
    [Show full text]
  • Dual-Mode Free-Jet Combustor
    Dual-Mode Free-Jet Combustor Charles J. Trefny and Vance F. Dippold III [email protected] NASA Glenn Research Center Cleveland, Ohio USA Shaye Yungster Ohio Aerospace Institute Cleveland, Ohio USA ABSTRACT The dual-mode free-jet combustor concept is described. It was introduced in 2010 as a wide operating-range propulsion device using a novel supersonic free-jet combustion process. The unique feature of the free-jet combustor is supersonic combustion in an unconfined free-jet that traverses a larger subsonic combustion chamber to a variable throat area nozzle. During this mode of operation, the propulsive stream is not in contact with the combustor walls and equilibrates to the combustion chamber pressure. To a first order, thermodynamic efficiency is similar to that of a traditional scramjet under the assumption of constant-pressure combustion. Qualitatively, a number of possible benefits to this approach are as follows. The need for fuel staging is eliminated since the cross-sectional area distribution required for supersonic combustion is accommodated aerodynamically without regard for wall pressure gradients and boundary-layer separation. The unconstrained nature of the free-jet allows for consideration of a detonative combustion process that is untenable in a walled combustor. Heat loads, especially localized effects of shock wave / boundary-layer interactions, are reduced making possible the use of hydrocarbon fuels to higher flight Mach numbers. The initial motivation for this scheme however, was that the combustion chamber could be used for robust, subsonic combustion at low flight Mach numbers. At the desired flight condition, transition to free-jet mode would be effected by increasing the nozzle throat area and inducing separation at the diffuser inlet.
    [Show full text]
  • A Comparison of Combustor-Noise Models – AIAA 2012-2087
    A Comparison of Combustor-Noise Models – AIAA 2012-2087 Lennart S. Hultgren, NASA Glenn Research Center, Cleveland, OH 44135 Summary The present status of combustor-noise prediction in the NASA Aircraft Noise Prediction Program (ANOPP)1 for current- generation (N) turbofan engines is summarized. Several semi-empirical models for turbofan combustor noise are discussed, including best methods for near-term updates to ANOPP. An alternate turbine-transmission factor2 will appear as a user selectable option in the combustor-noise module GECOR in the next release. The three-spectrum model proposed by Stone et al.3 for GE turbofan-engine combustor noise is discussed and compared with ANOPP predictions for several relevant cases. Based on the results presented herein and in their report,3 it is recommended that the application of this fully empirical combustor-noise prediction method be limited to situations involving only General-Electric turbofan engines. Long-term needs and challenges for the N+1 through N+3 time frame are discussed. Because the impact of other propulsion-noise sources continues to be reduced due to turbofan design trends, advances in noise-mitigation techniques, and expected aircraft configuration changes, the relative importance of core noise is expected to greatly increase in the future. The noise-source structure in the combustor, including the indirect one, and the effects of the propagation path through the engine and exhaust nozzle need to be better understood. In particular, the acoustic consequences of the expected trends toward smaller, highly efficient gas- generator cores and low-emission fuel-flexible combustors need to be fully investigated since future designs are quite likely to fall outside of the parameter space of existing (semi-empirical) prediction tools.
    [Show full text]
  • Comparison of Helicopter Turboshaft Engines
    Comparison of Helicopter Turboshaft Engines John Schenderlein1, and Tyler Clayton2 University of Colorado, Boulder, CO, 80304 Although they garnish less attention than their flashy jet cousins, turboshaft engines hold a specialized niche in the aviation industry. Built to be compact, efficient, and powerful, turboshafts have made modern helicopters and the feats they accomplish possible. First implemented in the 1950s, turboshaft geometry has gone largely unchanged, but advances in materials and axial flow technology have continued to drive higher power and efficiency from today's turboshafts. Similarly to the turbojet and fan industry, there are only a handful of big players in the market. The usual suspects - Pratt & Whitney, General Electric, and Rolls-Royce - have taken over most of the industry, but lesser known companies like Lycoming and Turbomeca still hold a footing in the Turboshaft world. Nomenclature shp = Shaft Horsepower SFC = Specific Fuel Consumption FPT = Free Power Turbine HPT = High Power Turbine Introduction & Background Turboshaft engines are very similar to a turboprop engine; in fact many turboshaft engines were created by modifying existing turboprop engines to fit the needs of the rotorcraft they propel. The most common use of turboshaft engines is in scenarios where high power and reliability are required within a small envelope of requirements for size and weight. Most helicopter, marine, and auxiliary power units applications take advantage of turboshaft configurations. In fact, the turboshaft plays a workhorse role in the aviation industry as much as it is does for industrial power generation. While conventional turbine jet propulsion is achieved through thrust generated by a hot and fast exhaust stream, turboshaft engines creates shaft power that drives one or more rotors on the vehicle.
    [Show full text]
  • 2. Afterburners
    2. AFTERBURNERS 2.1 Introduction The simple gas turbine cycle can be designed to have good performance characteristics at a particular operating or design point. However, a particu­ lar engine does not have the capability of producing a good performance for large ranges of thrust, an inflexibility that can lead to problems when the flight program for a particular vehicle is considered. For example, many airplanes require a larger thrust during takeoff and acceleration than they do at a cruise condition. Thus, if the engine is sized for takeoff and has its design point at this condition, the engine will be too large at cruise. The vehicle performance will be penalized at cruise for the poor off-design point operation of the engine components and for the larger weight of the engine. Similar problems arise when supersonic cruise vehicles are considered. The afterburning gas turbine cycle was an early attempt to avoid some of these problems. Afterburners or augmentation devices were first added to aircraft gas turbine engines to increase their thrust during takeoff or brief periods of acceleration and supersonic flight. The devices make use of the fact that, in a gas turbine engine, the maximum gas temperature at the turbine inlet is limited by structural considerations to values less than half the adiabatic flame temperature at the stoichiometric fuel-air ratio. As a result, the gas leaving the turbine contains most of its original concentration of oxygen. This oxygen can be burned with additional fuel in a secondary combustion chamber located downstream of the turbine where temperature constraints are relaxed.
    [Show full text]
  • Sir Frank Whittle
    Daniel Guggenheim Medal MEDALIST FOR 1946 For pioneering the development of turbojet propulsion of aircraft. SIR FRANK WHITTLE One day in July 1942, during World War II, a slightly-built young Englishman arrived in Washington on a highly confidential mission. So important was the equipment that accompanied him, so vital its secret, that he traveled under an assumed name and many who met him knew him only as “Frank.” He was in fact Frank Whittle, then a Wing Commander in the Royal Air Force; pioneer of the turbojet engine which was destined to make one of the most pro-found changes in aircraft propulsion since the beginning of powered flight. Born in Coventry, England, on June 1, 1907, Whittle entered Leamington College at the age of 11 on a scholarship won in elementary school. At the age of 16 he entered the Royal Air Force as an aircraft apprentice in the trade of metal rigger. At the final examination he was granted a cadetship at the Royal Air Force College, Cranwell. During 1928 and 1929, as a pilot officer, he spent fifteen months in the lllth Fighter Squadron and was then assigned to a flying instructors’ course at the Central Flying School, Wittering. It was during this course that the idea of using the turbine for jet propulsion first occurred to him. His patent application was filed in January, 1930. After one year as flying instructor and eighteen months as a floatplane and catapult testpilot, he was sent to Henlow in 1932 to take the Officers Engineering Course. The summer of 1934 saw him at Cambridge University (Peterhouse).
    [Show full text]
  • Novel Distributed Air-Breathing Plasma Jet Propulsion Concept for All-Electric High-Altitude Flying Wings
    Novel Distributed Air-Breathing Plasma Jet Propulsion Concept for All-Electric High-Altitude Flying Wings B. Goeksel1 IB Goeksel Electrofluidsystems, Berlin, Germany, 13355 The paper describes a novel distributed air-breathing plasma jet propulsion concept for all-electric hybrid flying wings capable of reaching altitudes of 100,000 ft and subsonic speeds of 500 mph, Fig. 1. The new concept is based on the recently achieved first breakthrough for air-breathing high-thrust plasma jet engines.5 Pulse operation with a few hundred Hertz will soon enable thrust levels of up to 5-10 N from each of the small trailing edge plasma thruster cells with one inch of core engine diameter and thrust-to-area ratios of modern fuel-powered jet engines. An array of tens of thrusters with a magnetohydrodynamic (MHD) fast jet core and low speed electrohydrodynamic (EHD) fan engine based on sliding discharges on new ultra-lightweight structures will serve as a distributed plasma “rocket” booster for a short duration fast climb from 50,000 ft to stratospheric altitudes up to 100,000 ft, Fig. 2. Two electric aircraft engines with each 110 lb (50 kg) weight and 260 kW of power as recently developed by Siemens will make the main propulsion for take-off and landing and climb up to 50,000 ft.3 4 Especially for climbing up to 100,000 ft the propellers will apply sophisticated pulsed plasma separation flow control methods. The novel distributed air-breathing plasma engine will be only powered for a short duration to reach stratospheric altitudes with lowest possible power consumption from the high-density battery swap modules and special fuel cell systems with minimum 660 kW, all system optimized for a short one to two hours near- space tourism flight application.2 The shining Plasma Stingray shown in Fig.
    [Show full text]
  • Reaction Engines and High-Speed Propulsion
    Reaction Engines and High-Speed Propulsion Future In-Space Operations Seminar – August 7, 2019 Adam F. Dissel, Ph.D. President, Reaction Engines Inc. 1 Copyright © 2019 Reaction Engines Inc. After 60 years of Space Access…. Copyright © 2019 Reaction Engines Inc. …Some amazing things have been achieved Tangible benefits to everyday life Expansion of our understanding 3 Copyright © 2019 Reaction Engines Inc. Accessing Space – The Rocket Launch Vehicle The rocket launch vehicle (LV) has carried us far…however current launchers still remain: • Expensive • Low-Operability • Low-Reliability …Which increases the cost of space assets themselves and restricts growth of space market …little change in launch vehicle technology in almost 60 years… 1957 Today 4 Copyright © 2019 Reaction Engines Inc. Why All-Rocket LV’s Could Use Help All-rocket launch vehicles (LVs) are challenged by the physics that dictate performance thresholds…little improvement in key performance metrics have been for decades Mass Fraction Propulsion Efficiency – LH2 Example Reliability 1400000 Stage 2 Propellant 500 1.000 Propellent 450 1200000 Vehicle Structure 0.950 236997 400 1000000 350 0.900 300 800000 0.850 250 Launches 0.800 600000 320863 200 906099 150 400000 Orbital Successful 0.750 100 Hydrogen Vehicle Weights (lbs) Weights Vehicle 0.700 LV Reliability 454137 (seconds)Impulse 200000 50 Rocket Engines Hydrogen Rocket Specific Specific Rocket Hydrogen 0 0.650 0 48943 Falcon 9 777-300ER 1950 1960 1970 1980 1990 2000 2010 2020 1950 1960 1970 1980 1990 2000 2010 2020 Air-breathing enables systems with increased Engine efficiency is paramount but rocket Launch vehicle reliability has reached a plateau mass margin which yields high operability, technology has not achieved a breakthrough in and is still too low to support our vision of the reusability, and affordability decades future in space 5 Copyright © 2019 Reaction Engines Inc.
    [Show full text]